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| { | |
| "schema_version": 1, | |
| "title": "Reproduction: Thinned Mean Field Langevin Dynamics", | |
| "emoji": "๐", | |
| "space_id": "snaykey/repro-thinned-mfld", | |
| "paper": { | |
| "openreview_id": "tt4UrPSGTo" | |
| }, | |
| "tags": [ | |
| "icml2026-repro", | |
| "paper-tt4UrPSGTo" | |
| ], | |
| "updated_at": "2026-08-02T00:00:00+00:00", | |
| "root": { | |
| "slug": "index", | |
| "title": "Reproduction: Thinned Mean Field Langevin Dynamics", | |
| "file": "pages/index.md", | |
| "children": [ | |
| { | |
| "slug": "claim-1-kt-mfld-complexity", | |
| "title": "KT-MFLD (Kernel-Thinned Mean Field Langevin Dynamics) reduces per-iteration computational complexity from O(N^2) to O(N^{3/2}) by applying kernel thinning (kt-split-Compress) to reduce N particles to a coreset of size M=O(sqrt(N)) at each step (Section 3).", | |
| "file": "pages/claim-1-kt-mfld-complexity/page.md", | |
| "children": [] | |
| }, | |
| { | |
| "slug": "claim-2-thm33-error", | |
| "title": "Theorem 3.3 shows that for sufficiently large N and T with an appropriate step size, KT-MFLD's finite-particle approximation error scales as O(N^{-1}(log N)^3), matching standard MFLD up to logarithmic factors (Theorem 3.3).", | |
| "file": "pages/claim-2-thm33-error/page.md", | |
| "children": [] | |
| }, | |
| { | |
| "slug": "claim-3-assumptions", | |
| "title": "Assumptions 3.1 and 3.2 require boundedness, Lipschitzness, and convexity of q1, q2, R1, plus membership of q1 and the gradient of q2 in a reproducing kernel Hilbert space, and the paper verifies these hold for mean-field neural networks, MMD quantization, and predictively-oriented (PrO) posteriors (Section 3, Section 4).", | |
| "file": "pages/claim-3-assumptions/page.md", | |
| "children": [] | |
| }, | |
| { | |
| "slug": "claim-4-experiments", | |
| "title": "Experiments on student-teacher networks, MMD quantization, and PrO posteriors show KT-MFLD consistently outperforms random subsampling and random-batch baselines under equal computational budgets (Section 4).", | |
| "file": "pages/claim-4-experiments/page.md", | |
| "children": [] | |
| }, | |
| { | |
| "slug": "claim-5-curse-of-dimensionality", | |
| "title": "The authors note the thinning-induced error term suffers a curse of dimensionality, since the constant term can be exponentially small in dimension d, worsening particle-complexity dependence in high dimensions (Section on limitations).", | |
| "file": "pages/claim-5-curse-of-dimensionality/page.md", | |
| "children": [] | |
| }, | |
| { | |
| "slug": "executive-summary", | |
| "title": "executive-summary", | |
| "file": "pages/executive-summary/page.md", | |
| "children": [] | |
| }, | |
| { | |
| "slug": "conclusion", | |
| "title": "conclusion", | |
| "file": "pages/conclusion/page.md", | |
| "children": [] | |
| } | |
| ] | |
| } | |
| } |